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Abstracts - KTH Mechanics

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3D chaotic mixing inside drops driven by transient electric field<br />

Xiumei Xu a and G. M. Homsy a<br />

We study the 3D chaotic trajectories inside a neutrally buoyant drop driven by<br />

periodically switching a uniform electric field through an angle . The extent of the<br />

chaotic mixing is related to two parameters: the angle and modulation period T. In a<br />

static electric field, the streamlines internal to the drop are axisymmetric Taylor<br />

circulations with two rings of center fixed points (CFP) at the top and bottom<br />

hemispheres corresponding to the vortex center. Periodically switching the field is<br />

equivalent to periodically changing the axis of symmetry, and thus the position of<br />

these CFPs. There are always common CFPs during the field rotation, and there are<br />

either 4 or 8 depending on the range of . When equals /2, although the<br />

trajectories are three dimensional, Poincare maps show that for all modulating periods,<br />

the 3D trajectories are confined to certain KAM surfaces, determined only by initial<br />

positions, which limit the mixing. For other than /2, chaotic mixing is generated<br />

inside the drop, but there are ordered regions near the common CFPs, with more<br />

regions for the larger number of common CFPs (Figure 1). Inside the ordered regions,<br />

trajectories move around the common CFPs in complicated way, and the Poincare<br />

maps can exhibit highly ordered fractal structures. The mixing also depends on the<br />

modulating period, and our numerical results show that by modifying T it is possible<br />

to break the ordered islands and achieve global chaotic mixing. These results suggest<br />

there are optimum operating conditions that maximize mixing.<br />

a University of California-Santa Barbara, Santa Barbara, 93106, USA<br />

z<br />

(a) (b)<br />

z<br />

y y<br />

Figure 1: Typical Poincare maps, T=6, (a) =0.45 , the case of 8 common center<br />

fixed points; (b) =0.25 , the case of 4 common center fixed points.<br />

189

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